# Self-avoiding trails with nearest neighbour interactions on the square lattice

###### Abstract

Self-avoiding walks and self-avoiding trails, two models of a polymer coil in dilute solution, have been shown to be governed by the same universality class. On the other hand, self-avoiding walks interacting via nearest-neighbour contacts (ISAW) and self-avoiding trails interacting via multiply-visited sites (ISAT) are two models of the coil-globule, or collapse transition of a polymer in dilute solution. On the square lattice it has been established numerically that the collapse transition of each model lies in a different universality class.

The models differ in two substantial ways. They differ in the types of subsets of random walk configurations utilised (site self-avoidance versus bond self-avoidance) and in the type of attractive interaction. It is therefore of some interest to consider self-avoiding trails interacting via nearest neighbour attraction (INNSAT) in order to ascertain the source for the difference in the collapse universality class. Using the flatPERM algorithm, we have performed computer simulations of this model. We present numerical evidence that the singularity in the free energy of INNSAT at the collapse transition has a similar exponent to that of the ISAW model rather than the ISAT model. This would indicate that the type of interaction used in ISAW and ISAT is the source of the difference in universality class.

## 1 Introduction

The collapse transition of a polymer in a dilute solution has been a focus of study in lattice statistical mechanics for decades [1, 2]. Any lattice model of a collapsing polymer has two key ingredients: an excluded volume effect expressing the impenetrability of monomers, and a short-range attractive force, which mimics the complex monomer-solvent interaction. When the effects of the excluded volume and the short-range attraction balance each other, the polymer undergoes a collapse transition which separates two distinct phases: a swollen and a collapsed phase.

The canonical lattice model of the configurations of a polymer in solution has been the model of self-avoiding walks (SAW) where a random walk on a lattice is not allowed to visit a lattice site more than once. SAW display the desired excluded volume effect and are swollen in size relative to unrestricted random walks at the same length. A common way to introduce a short-range interaction is to assign a negative energy to each non-consecutive pair of monomers lying on neighbouring lattice sites, modelling an effective attractive force. This is the interacting self-avoiding walk (ISAW) model, which is the standard lattice model of polymer collapse using self-avoiding walks.

The properties of lattice polymers are also related to those of magnetic systems near their critical point [3]. More precisely, lattice polymers are related to magnets with symmetry in the formal limit of zero components (). This relation is of great importance, since it allows the application of the methods of statistical field theory to the study of polymer models, and the collapse transition can be understood as the tri-critical point of such systems [1, 4, 5].

The study of the critical properties of lattice polymers, and thus of models when we let , in two dimensions has been ongoing over decades theoretically and numerically. Nienhuis in 1982 [6] was able to compute the critical exponents of free SAW by considering a model of non-intersecting loops on the hexagonal lattice, and in 1987 Duplantier and Saleur [7] were able to model the bond interaction introducing vacancies on the same lattice, obtaining a full set of critical exponents for the polymer collapse transition in the ISAW model. Their conjectured values for the exponents have been subsequently confirmed numerically by Prellberg and Owczarek in 1994 [8]. We will refer to (the universality class of) this critical point as the ‘-point’.

Introducing attractive interactions between bonds opens the doors to more complex possibilities. In the quest for a solvable model on the square lattice, Blöte and Nienhuis in 1989 [9] considered a lattice model, which includes energies for site-collisions and straight segments. For this model five critical branches are exactly known [9, 10, 11, 12]. One of these branches (named ‘branch 0’ in [9]) is similar to the -point previously found by Duplantier and Saleur [7] (for this branch Batchelor [13] obtained the exponents , ), and two branches correspond to dense and dilute (SAW) polymers. The two remaining branches are, respectively, associated with a combination of Ising-like and critical behaviour and with a new tri-critical point. This new tri-critical point (with exponents , ) is another candidate for describing a collapsing polymer.

A different model of a collapsing model can be constructed starting from self-avoiding trails. A self-avoiding trail (SAT) is a lattice walk configuration where the excluded volume is obtained by preventing the walk from visiting the same bond, rather than the same site, more than once. This is a slightly weaker restriction, and SAW configurations are a proper subset of SAT configurations. The interacting version of self-avoiding trails (ISAT), customarily obtained by giving an energy to multiple visited sites, also presents a collapse transition.

It is known that SAW and SAT share the same statistics in their high-temperature phase, but theoretical prediction and numerical evidence [14, 15] strongly suggests that the collapse transition of the ISAT model is in a different universality class to that of ISAW, although there is no clear understanding of why this would be the case. An interesting possible explanation of the ISAT collapse has been provided by Foster [16] in terms of the tri-critical point with exponents , derived from the model.

Although they both aim to describe the same physical system, the ISAW and ISAT models differ in both their geometrical properties and their interaction. Their different critical behaviour could be due to either one of these two differences.

To investigate this further, we considered a mixed model where trails interact in the same way as SAW, that is, by a nearest-neighbour interaction. We shall call this new hybrid model Interacting Nearest-Neighbour Self-Avoiding Trails, or INNSAT. In the next section we review the ISAW and ISAT models describing the different behaviours that they have been shown to demonstrate. In Section 3 we formally introduce our new model INNSAT and the quantities of interest. We then describe our results in Section 4 and summarise our conclusions in the final section.

## 2 ISAW and ISAT

### 2.1 Interacting Self-Avoiding Walks (ISAW)

Let us recall briefly the definition and main properties of the ISAW model. Consider the ensemble of self-avoiding walks (SAW) of length , that is, of all lattice paths of steps that can be formed on the square lattice such that they never visit the same site more than once. Given a SAW , we define a contact whenever there is a pair of sites that are neighbours on the lattice but not consecutive on the walk. We associate an energy with each contact. Denoting by the number of contacts in , the probability of is given by

(2.1) |

and the partition function is defined in the usual way as

(2.2) |

where is the inverse temperature ( is Boltzmann’s constant). We define a Boltzmann weight (fugacity) . The finite-length reduced free energy is

(2.3) |

and the thermodynamic limit is obtained by taking the limit of large , i.e.,

(2.4) |

As mentioned above, it is expected that there is a collapse phase transition at a temperature , which is known as the -point, characterised by a non-analyticity in .

The temperature also separates regions of different finite-length scaling behaviour for fixed temperatures. Considering this finite-length scaling, for high temperatures () the excluded volume interaction is the dominant effect, and the behaviour is universally the same as for the non-interacting SAW problem: for large , the mean squared end-to-end distance (or equivalently the radius of gyration) and partition function are expected to scale as

(2.5) | ||||

(2.6) |

respectively, where and the exponents and are expected to be universal. In two dimensions it is well established [6] that and for . The constants and are temperature dependent.

Fixing the temperature precisely at the -point, , Duplantier and Saleur [7] found and in two dimensions.

For low temperatures () it is accepted that the partition function is dominated by configurations that are internally dense, though not necessarily fully dense. The partition function should then scale differently from that at high temperatures, since a collapsed polymer should have a well-defined surface (and associated surface free energy) [17]. One expects in dimensions large- asymptotics of the form

(2.7) | ||||

(2.8) |

with . The constants and are temperature dependent. It is expected that the internal density smoothly goes to zero as the temperature is raised to the -point.

To explore the singularity in the free energy at the collapse point further, it is useful to consider the (reduced) internal energy and the specific heat, which are defined as

(2.9) |

with limits

(2.10) |

When , the singular part of the specific heat behaves as

(2.11) |

where for a second-order phase transition. If the transition is second-order, the singular part of the thermodynamic limit internal energy behaves as

(2.12) |

when , and there is a jump in the internal energy at if the transition is first-order (an effective value of ).

Tri-critical scaling [18] predicts that around the critical temperature, the finite-length scaling of the singular part of the specific-heat obeys the following crossover scaling form

(2.13) |

when and , and that the exponents and are related via

(2.14) |

If one considers the peak of the finite-length specific heat it will behave as

(2.15) |

where is the location of the maximum of the function .

The work of Duplantier and Saleur (1987) predicts the exponents for the -point collapse are

(2.16) |

and

(2.17) |

It is important to observe that this implies that the specific heat does not diverge at the transition since the exponent

(2.18) |

is negative. However, the peak values of the third derivative of the free energy with respect to temperature will diverge with positive exponent

(2.19) |

### 2.2 Interacting Self-Avoiding Trails (ISAT)

The model of interacting trails on the square lattice is defined as follows. Consider the ensemble of self-avoiding trails (SAT) of length , that is, of all lattice paths of steps that can be formed on the square lattice such that they never visit the same bond more than once. Given a SAT , we associate an energy with each doubly visited site. Denoting by the number of doubly visited sites in , the probability of is given by

(2.20) |

where we define the Boltzmann weight and the partition function of the ISAT model is given by

(2.21) |

Previous work [14, 15] on the square lattice has shown that there is a collapse transition at a temperature with a strongly divergent specific heat, and the exponents have been estimated as

(2.22) |

arising from a scaling of the peak value of the specific heat diverging with exponent

(2.23) |

This result is a clear difference to the ISAW -point described above where the singularity in the specific heat is convergent. Additionally, at the finite-length scaling of the end-to-end distance was found to be consistent [14] with the form

(2.24) |

as . Again, this is quite different to the exponent for the ISAW.

Another important difference is that it has been recently observed [19, 20] that the low temperature phase is maximally dense on the triangular and square lattices. On the square lattice this implies that if one considers the proportion of the sites on the trail that are at lattice sites which are not doubly occupied via

(2.25) |

then it is expected that

(2.26) |

## 3 The INNSAT model

We define our new interacting model of trails (INNSAT) as follows. Consider the set of bond-avoiding paths as defined in the previous section. When two sites are adjacent on the lattice but not consecutive along the walk, so as not to be joined by any step of the walk, we again refer to this pair of sites as a nearest-neighbour contact and we give it a weight , analogously to the ISAW model. In Figure 1 a trail of length with contacts is illustrated.

Denoting by the number of contacts in , the probability of is given by

(3.1) |

where the partition function is

(3.2) |

The intensive reduced internal energy and specific heat are as for ISAW:

(3.3) |

We shall also consider the proportion of the sites on the trail that are at lattice sites which are not doubly occupied via

(3.4) |

where is the number of doubly visited sites as defined above.

We shall see there is a collapse transition at a single temperature, , equivalently, fugacity . If the INNSAT model behaves in the same way as the ISAW model we would not expect the specific heat to diverge at this collapse point so we also need to introduce a quantity proportional to the third derivative of the free energy as

(3.5) |

This quantity should have a singular part that behaves as

(3.6) |

around the collapse point, i.e., as and . Hence the peaks of this quantity will scale with exponent .

## 4 Numerical Results

We have first simulated the INNSAT model using the flatPERM algorithm [21] up to length . With iterations, we collected samples at the maximum length. Following [21], we also measured the number of samples adjusted by the number of their independent growth steps, obtaining “effective samples”.

FlatPERM outputs an estimate of the total weight of the walks of length at fixed values of . From the total weight one can access physical quantities over a broad range of temperatures through a simple weighted average, e.g.

(4.1) |

We have begun by analysing the scaling of the specific heat by calculating the location of its peak and thereby evaluating . We have also found the two peaks of as a function of temperature: the peak values we denote .

It is clear that the specific heat peak is growing rather weakly as length increases. As the specific heat might converge, we obtain finite size estimates of the specific heat exponent by considering

(4.2) |

which should converge to as . Assuming corrections to scaling of as for ISAW, we find

(4.3) |

as shown on the left-hand side of Figure 2. This is consistent with a value of for the -point universality class.

Furthermore when we analyse , which is proportional to the third derivative of the free energy, we find further consistent values of exponents. This derivative has two peaks , and we obtain finite size estimates of the specific heat exponent from each of the peaks by considering

(4.4) |

which should converge to as . From the plot on the right-hand side of Figure 2 we estimate

(4.5) |

There is still considerable curvature in the right-hand plot which would indicate a slightly larger value when higher order corrections to scaling are taken in account. Once again we conclude that the value of is consistent with our data.

We therefore conjecture that

(4.6) |

Using the locations of the peaks of the specific heat and its derivative and assuming finite-size correction of the order of , we have estimated the location of the collapse point as indicated in Figure 3. The magnitude of the difference between the three peak positions at finite length indicates the large corrections to scaling present in this problem at length . We estimate

(4.7) |

We next analysed the scaling of the end-to-end distance of the polymer. To obtain an estimate for the exponent we considered a finite-size effective exponent

(4.8) |

Using the data obtained from our flatPERM simulations, we plotted this quantity against temperature for various values of the length , as shown in Figure 4. We find that the graphs for different values of intersect around a particular value of the temperature. The location of this intersection point is a good estimator of the infinite-length critical temperature and of the exponent at the transition. We find a region of crossing points in between and with corresponding estimates of between and . While the obtained exponent estimate range is a little below the point value of , we expect that our estimate is affected by strong corrections to scaling. For comparison, we simulated the ISAW model and performed an identical analysis, shown in Figure 5. The ISAW estimate of at the collapse transition, while being closer to 4/7, also indicates the presence of strong corrections to scaling.

Hence, we ran a thermal simulation at the estimated critical fugacity of up to . With iterations, we obtained samples at the maximum length (corresponding to “effective samples”). Figure 6 shows a log-log plot of the radius with respect to the size of the walk along with a linear best fit with slope 0.575. Of course, using or gives estimates of that differ by so the sensitivity to the location of the critical point dominates the error of our estimate.

Correspondingly, if we assume that the INNSAT is in the ISAW universality class we can use the value of to better estimate the critical fugacity in the INNSAT model as

(4.9) |

### 4.1 Low-temperature phase

There is strong evidence that the low-temperature phase of the ISAW model is a globular phase that is not fully dense, while for interacting trails the low-temperature phase is maximally dense. As discussed above, the trail fills the lattice asymptotically in a maximally dense phase, and the portion of steps not involved with doubly-visited sites should tend to zero as . Following the analysis in [19] we measured the proportion of steps visiting the same site twice, and we plotted against at two different temperatures respectively above and below the critical temperature, as shown in Figure 7). We find that in both low-temperature and high-temperature phases only a small portion of the visited sites is visited again. The quantity stays close to 1 and, in particular, does not tend to zero in either region. This phenomenon can be understood by noting that the nearest-neighbour interaction makes energetically favourable for the walk to bounce away from an already visited site rather than to visit it again.

This result implies that the low temperature phase is not fully dense, just as for the ISAW low temperature phase. This provides a consistent picture that the collapse transition in the INNSAT model is between high and low temperature phases similar to the ISAW, making the conclusion that the thermodynamic transition between them is similar to the -point a natural one.

## 5 Conclusions

We have considered a new lattice model of polymer collapse in two dimensions which uses the interaction type, nearest neighbour contacts, of the canonical lattice model (ISAW) but the configuration space of an alternative model (ISAT), being bond-avoiding walks, also known as self-avoiding trails. We find that the critical behaviour of the free energy, and its derivatives of our model (INNSAT) seems to align with the -point universality class of the ISAW model rather than that of the ISAT model, which has rather a strongly divergent specific heat not seen in either the ISAW or INNSAT models. The end-to-end distance scaling is broadly consistent with this conclusion, though estimates tend to be a little low. However, using the assumption that the INNSAT and ISAW models lie in the same universality class leads to a precise estimate of the critical fugacity as . Given the different universality classes for ISAT and INNSAT it may also be of interest to consider a model based upon self-avoiding trail configurations with both types of interaction.

## Acknowledgements

Financial support from the Australian Research Council via its support for the Centre of Excellence for Mathematics and Statistics of Complex Systems and through its Discovery Program is gratefully acknowledged by the authors. A L Owczarek thanks the School of Mathematical Sciences, Queen Mary, University of London for hospitality.

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